17.12.2012 Views

IRAC Instrument Handbook - IRSA - California Institute of Technology

IRAC Instrument Handbook - IRSA - California Institute of Technology

IRAC Instrument Handbook - IRSA - California Institute of Technology

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

<strong>IRAC</strong> <strong>Instrument</strong> <strong>Handbook</strong><br />

Figure 4.6. The <strong>IRAC</strong> point res ponse functions (PRFs) at 3.6, 4.5, 5.8 and 8.0 microns. The PRFs were<br />

generated from models refined with in-flight calibration test data invol vi ng a bright cali brati on star observed<br />

at several epochs. Central PRFs for each channel are shown above wi th a logarithmic scaling to hel p dis play<br />

the entire dynamic range. The PRFs are shown as they appear with 1/5th the native <strong>IRAC</strong> pixel sampling <strong>of</strong><br />

1.2 arcseconds to highlight the core structure.<br />

4.7.2 Extended PRFs<br />

The FITS files <strong>of</strong> the extended PRFs can be obtained using the links in the <strong>IRAC</strong> web pages. In order to<br />

gain high signal-to-noise out to the edge <strong>of</strong> the arrays, PRFs were generated from a combination <strong>of</strong> onboard<br />

calibration and science observations <strong>of</strong> stars with different brightness, joined together to produce<br />

extended high dynamic range (HDR) observational PRFs. These PRFs have two main components: a core<br />

HDR PRF created by the observations <strong>of</strong> a reference star, and the extended region from observations <strong>of</strong> a<br />

set <strong>of</strong> bright stars that saturated the <strong>IRAC</strong> array. They can be used to perform source extraction and PRFfitting<br />

photometry <strong>of</strong> bright, highly saturated stars with extended wings. The core <strong>of</strong> the extended PRF<br />

was generated using the prf_estimate module <strong>of</strong> MOPEX which has been shown to be inadequate for<br />

making high-quality PRFs for <strong>IRAC</strong>. As a result, the extended PRF should not be used for PRF-fitting<br />

photometry and source extraction <strong>of</strong> non-saturated point sources. Instead, the core PRF in Section 4.7.1 is<br />

more appropriate for PRF-fitting photometry. Also, note that the detailed structure <strong>of</strong> the center <strong>of</strong><br />

saturated sources fitted using the extended PRF will not be correct in detail.<br />

These extended HDR PRFs have a pixel size <strong>of</strong> 0.2 <strong>IRAC</strong> pixels, or ~ 0.24 arcsec. The size <strong>of</strong> each PRF<br />

image is 1281x1281 pixels, covering an area <strong>of</strong> ~ 5.1 arcmin x 5.1 arcmin. The PRFs are centered within<br />

each image. The PRFs are calibrated in MJy/sr. The PRFs represent an unsaturated, very high S/N image<br />

<strong>of</strong> Vega, and the flux density contained within a 10 native <strong>IRAC</strong> pixel aperture radius (50 HDR PRF<br />

pixels), with the sky level estimated in a radial annulus from 12 to 20 native <strong>IRAC</strong> pixels, is equal to the<br />

flux density <strong>of</strong> Vega. The pedestal level <strong>of</strong> each image is set to zero in the corners <strong>of</strong> each PRF.<br />

To produce the core portion <strong>of</strong> the HDR PRF, 300 HDR observations <strong>of</strong> a calibration star were obtained<br />

during three separate epochs, each observation consisting <strong>of</strong> short exposures (0.6 sec/1.2 sec) and long<br />

exposures (12 sec/30 sec). The HDR PRFs were generated by first combining short-exposure frames and<br />

long-exposure frames separately. The short frames enabled the cores to be constructed without a<br />

saturation problem, while the long exposures allowed the construction <strong>of</strong> a higher signal-to-noise PRF in<br />

the wings out to 15 arcseconds. The assembly required the replacement <strong>of</strong> any saturated areas in the longexposure<br />

frames with unsaturated data from the same pixel area <strong>of</strong> the short-exposure frames. It also<br />

required the replacement <strong>of</strong> a few pixels in the long-exposure frames by the corresponding pixels in the<br />

short-exposure frames to mitigate the non-linear bandwidth effect in channels 3 and 4. The "stitching" <strong>of</strong><br />

the two components <strong>of</strong> the HDR PRF was completed using a 1/r masking algorithm requiring a<br />

percentage <strong>of</strong> each frame to be added together over a small annulus two <strong>IRAC</strong> pixels in width just outside<br />

the saturated area. Each epoch was treated separately and then all three epochs were aligned and a median<br />

was taken to remove background stars.<br />

Calibration 49 <strong>IRAC</strong> Point Spread and Point<br />

Response Functions

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!